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A \(7.00-\mu \mathrm{F}\) capacitor is initially charged to a potential of 16.0 \(\mathrm{V}\) . It is then connected in series with a 3.75 -mH inductor. (a) What is the total energy stored in this circuit? (b) What is the maximum current in the inductor? What is the charge on the capacitor plates at the instant the current in the inductor is maximal?

Short Answer

Expert verified
(a) The total energy stored is \(8.96 \times 10^{-4}\text{ J}\). (b) The maximum current in the inductor is approximately \(0.691\text{ A}\), and the charge on the capacitor is \(0\text{ C}\).

Step by step solution

01

Calculate the Energy in the Capacitor

The energy stored in the capacitor when it is charged is given by the formula: \[ U = \frac{1}{2} C V^2 \]where \( C = 7.00 \times 10^{-6} \text{ F} \) and \( V = 16.0 \text{ V} \).Plug in these values:\[ U = \frac{1}{2} \times 7.00 \times 10^{-6} \times (16.0)^2 \]\[ U = \frac{1}{2} \times 7.00 \times 10^{-6} \times 256 \]\[ U = 8.96 \times 10^{-4} \text{ J} \]
02

Determine the Maximum Current in the Inductor

The maximum current \( I_{max} \) in the inductor is when all the energy initially stored in the capacitor is converted into kinetic energy of the inductance. This is given by:\[ U = \frac{1}{2} L I_{max}^2 \]where \( L = 3.75 \times 10^{-3} \text{ H} \).Solve for \( I_{max} \):\[ 8.96 \times 10^{-4} = \frac{1}{2} \times 3.75 \times 10^{-3} \times I_{max}^2 \]\[ I_{max}^2 = \frac{2 \times 8.96 \times 10^{-4}}{3.75 \times 10^{-3}} \]\[ I_{max}^2 = 0.4778 \]\[ I_{max} = \sqrt{0.4778} \]\[ I_{max} \approx 0.691 \text{ A} \]
03

Determine the Charge on the Capacitor at Maximum Inductor Current

At maximum current in the inductor, the charge on the capacitor is zero because all the energy is transferred to the inductor. Therefore, the charge on the capacitor plates at the instant the current in the inductor is maximal is:\[ q = 0 \text{ C} \].

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Energy Storage in Capacitors
When a capacitor is charged, it stores energy in an electric field between its plates. This energy can be calculated using the formula: \[ U = \frac{1}{2} C V^2 \]where \( U \) is the stored energy, \( C \) is the capacitance, and \( V \) is the voltage across the capacitor. In simple terms, this formula tells us that the energy depends on both how much charge the capacitor can hold (capacitance), and the potential difference between its plates (voltage). For example, using the given values from the exercise, a capacitor with a capacitance of 7.00 \( \mu \mathrm{F} \) and a voltage of 16.0 V can store a total energy of 0.000896 Joules after calculation.
  • Capacitance (\( C \)) affects how much charge can be stored.
  • Voltage (\( V \)) influences the amount of energy stored.
This stored energy is crucial because it can be later transferred to other components in the circuit, such as an inductor.
Maximum Inductor Current
In an LC circuit, when an initially charged capacitor is connected to an inductor, the energy stored in the capacitor is gradually transferred to the inductor. At the moment when all this energy has shifted completely into the inductor, the current through the inductor reaches its maximum value.This maximum inductor current can be calculated using the equation for energy conservation:\[ U = \frac{1}{2} L I_{\text{max}}^2 \]Here, \( U \) is the same energy initially stored in the capacitor, \( L \) is the inductance, and \( I_{\text{max}} \) is the maximum current.By rearranging and solving, we find \( I_{\text{max}} \) to be approximately 0.691 A, using the inductance of 3.75 mH. The initial energy from the capacitor's electric field fully converts into magnetic energy in the inductor at this point.
  • Maximum current is reached when all energy is transferred to the inductor.
  • The formula relates energy with inductance and current.
Charge on Capacitor Plates
In an LC circuit, the charge and current are dynamically changing due to the continuous energy exchange between the capacitor and the inductor. At the moment when the current through the inductor is at its maximum, the charge on the capacitor plates is zero. Why is this? Because all the energy stored in the capacitor has been converted to kinetic energy in the form of the current flowing through the inductor.Thus, the charge (\( q \)) on the capacitor is:\[ q = 0 \text{ C} \]at that instant. There are different stages in this energy oscillation, but at this specific moment, energy rests only in the inductor.
  • Charge is zero when maximum current flows through the inductor.
  • Energy forms a cycle between the capacitor and the inductor.

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Most popular questions from this chapter

An inductor used in a dc power supply has an inductance of 12.0 \(\mathrm{H}\) and a resistance of 180\(\Omega .\) It carries a current of 0.300 \(\mathrm{A}\) . (a) What is the energy stored in the magnetic field? (b) At what rate is thermal energy developed in the inductor? (c) Does your answer to part (b) mean that the magnetic-field energy is decreasing with time? Explain.

An inductor with an inductance of 2.50 \(\mathrm{H}\) and a resistance of 8.00\(\Omega\) is connected to the terminals of a battery with an emf of 6.00 \(\mathrm{V}\) and negligible internal resistance. Find (a) the initial rate of increase of current in the circuit; (b) the rate of increase of current at the instant when the current; is \(0.500 \mathrm{A} ;\) (c) the current 0.250 \(\mathrm{s}\) after the circuit is closed; (d) the final steady-state current.

At the instant when the current in an inductor is increasing at a rate of \(0.0640 \mathrm{A} / \mathrm{s},\) the magnitude of the self-induced emf is 0.0160 \(\mathrm{V}\) (a) What is the inductance of the inductor? (b) If the inductor is a solenoid with 400 turns, what is the average magnetic flux through each turn when the current is 0.720 \(\mathrm{A} ?\)

An inductor is connected to the terminals of a battery that has an emf of 12.0 \(\mathrm{V}\) and negligible internal resistance. The current is 4.86 \(\mathrm{mA}\) at 0.940 \(\mathrm{ms}\) after the connection is completed. After a long time the current is 6.45 \(\mathrm{mA} .\) What are (a) the resistance \(R\) of the inductor and (b) the inductance \(L\) of the inductor?

A toroidal solenoid with mean radius \(r\) and cross-sectional area \(A\) is wound uniformly with \(N_{1}\) turns. A second toroidal solenoid with \(N_{2}\) turns is wound uniformly on top of the first, so that the two solenoids have the same cross-sectional area and mean radius. (a) What is the mutual inductance of the two solenoids? Assume that the magnetic field of the first solenoid is uniform across the cross section of the two solenoids. (b) If \(N_{1}=500\) turns, \(N_{2}=300\) turns, \(r=10.0 \mathrm{cm},\) and \(A=0.800 \mathrm{cm}^{2},\) what is the value of the mutual inductance?

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